provided that the potential \(V(r)\)  can be expressed in the generic form \(V(r)=\epsilon f(r/\sigma )\) , where \(f(r)\)  is a well-defined dimensionless interaction function and \(\Lambda \equiv \hbar /(\sigma \sqrt{\mu \epsilon })\)  [1]}. From (REF ) we see that \(\Lambda \) , the so-called De Boer parameter, is the only parameter in the equation that gives information about the particular microscopic characteristics of the system. From this fact, De Boer was able to formulate his principle of corresponding states, which is a “quantum” generalization of the van der Waals law of corresponding states for classical gases and liquids [2]}, [3]}, [4]}. The De Boer principle of corresponding states tells us that two different systems with equal value of \(\Lambda \)  have identical thermodynamic properties [1]}. In Section  we exploit this principle in order to give an interpretation to the supersymmetric integrable model for zero energy, we propose with the \(10-6\)  Lennard-Jones potential.
